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section of a fiber bundle
Let $\funcdef{p}{E}{B}$ be a fiber bundle, denoted by $\xi.$
A section of $\xi$ is a continuous map $\funcdef{s}{B}{E}$ such that the composition $p\comp s$ equals the identity. That is, for every $b\in B,$ $s(b)$ is an element of the fiber over $b.$ More generally, given a topological subspace $A$ of $B,$ a section of $\xi$ over $A$ is a section of the restricted bundle $\funcdef{\restr{p}{A}}{\inv{p}(A)}{A}.$
The set of sections of $\xi$ over $A$ is often denoted by $\Gamma(A;\xi),$ or by $\Gamma(\xi)$ for sections defined on all of $B.$ Elements of $\Gamma(\xi)$ are sometimes called global sections, in contrast with the local sections $\Gamma(U;\xi)$ defined on an open set $U.$
In fact, any tensor field on a smooth manifold $M$ is a section of an appropriate vector bundle. For instance, a contravariant $k$ -tensor field is a section of the bundle $TM^{\otimes k}$ obtained by repeated tensor product from the tangent bundle, and similarly for covariant and mixed tensor fields.
It is interesting to ask if a vector bundle admits a section which is nowhere zero. The answer is yes, for example, in the case of a trivial vector bundle, but in general it depends on the topology of the spaces involved. A well-known case of this question is the hairy ball theorem, which says that there are no nonvanishing tangent vector fields on the sphere.
